EP0365084A1

EP0365084A1 - Computer tomography scanner with a tomosynthetic scanogram

Info

Publication number: EP0365084A1
Application number: EP89202578A
Authority: EP
Inventors: Willem Peter Van Der Brug; Jan Timmer; Petrus Nicolaas Joseph Vis
Original assignee: Philips Gloeilampenfabrieken NV; Koninklijke Philips Electronics NV
Current assignee: Koninklijke Philips NV
Priority date: 1988-10-18
Filing date: 1989-10-12
Publication date: 1990-04-25
Also published as: US5060246A; JPH02156931A; IL91998A0; NL8802556A

Abstract

In a computer tomography device comprising an X-ray tube having an elongate anode across which a focus can be displaced, a tomosynthetic scanogram can be formed by correctly shifting the profiles measured in the various source positions with respect to one another, followed by superposition. Parts of the object which are situated in a selected layer are thus emphasized in an image, parts of the object which are situated outside the selected layer being blurred. An important additional advantage consists in that the permissible power to be applied to the X-ray source may be higher. Furthermore, a scanogram thus obtained is not necessarily disturbed by the failure of one or more detectors.

Description

The invention relates to a computer tomography device for determining a radiation absorption distribution in a transverse slice of an object, which device comprises an X-ray source and detector means for irradiating the object from a plurality of different directions and for detecting the radiation having passed the object, and also comprises an object carrier and displacement means for displacing the object and the object carrier in a direction transversely of the irradiation direction of the X-ray source.
A computer tomography device of this kind is known from German Patent Application 26 13 809. Via the object carrier, the object is displaced transversely of the irradiation direction of the radiation source by the displacement means, the radiation source and the detector means occupying a stationary position, in order to obtain a two-dimensional shadow image of the object. This two-dimensional shadow image enables the determination of position of an object slice for which an absorption distribution is to be determined. Such a two-dimensional shadow image is referred to as a scanogram hereinafter. Like any other shadow image formed by means of a conventional X-ray apparatus, a scanogram has the drawback that the various parts of an object, situated above one another when looking in the direction from the detector to the X-ray source, are imaged in a superposed fashion in a shadow image. As a result, one part of the object may completely mask another part of the object. Due to such masking, the scanogram fails to offer sufficient information for making a slice image of the object in the desired location.
The invention has for its object to provide a computer tomography device enabling the formation of a scanogram in which the information can be emphasized in a given layer which extends transversely of the irradiation direction of the X-ray source.
To achieve this, the computer tomography device in accordance with the invention is characterized in that after a translation of the object, the X-ray source is always situated at the same side of the object so as to irradiate the object from different directions, the device also comprising arithmetic means for combining the detector signals, generated in said different directions, so as to obtain a semi-scanogram in which an object layer is emphasized which is to be selected in advance and which extends substantially transversely of the plane of the irradiation directions.
It is to be noted that a computer tomography device comprising an X-ray tube having an elongate anode which is scanned by an electron beam is known from German Patent Application 25 51 322; however, the scanning motion of the electron beam on the anode thereof always takes place simultaneously with the rotary motion of the X-ray source and the detector means around the object in order to achieve a desired measuring path distribution within the object for the reconstruction of a transverse slice image thereof.
The invention will be described in detail hereinafter with reference to the drawing; therein

Fig. 1 diagrammatically shows a device in accordance with the invention,
Fig. 2 is a geometrical illustration of the calculation of a tomosynthetic scanogram, and
Fig. 3 diagrammatically shows the geometry of the invention for determining the blurring factor in a tomosynthetic scanogram.

Fig. 1 shows a computer tomography device in accordance with the invention, comprising an X-ray source 1 having an elongate anode 3 for generating a diverging, flat X-ray beam 4 which, after having passed an object 5 arranged on an object carrier 7, is detected by an array of detectors 9. Through the detection of X-rays the detectors 9 generate signals which are stored by a processing device 11 The object carrier 7 can be displaced by translation means 13 in a direction which is denoted by the reference L and which extends transversely of the radiation of the X-ray source 1. The computer tomography device 10 also comprises a control unit 15 which generates control signals for the high-voltage unit 17, the translation means 13 and the processing unit 11 in order to synchronize the generating of the X-ray beam, the translation and the processing of the measuring signals generated by the detectors 9. From the detector signals the processing unit 11 calculates a scanogram which is displayed on a display device 19. It will be evident that the tomography device 10 comprises known rotation means for rotating the X-ray source 1 and the detector means 9 around the object 5 in order to make a sectional image of the radiation absorption distribution in a plane 8 defined by the flat, diverging beams 4. Such rotation means and the processing of the signals thus generated are known and will not be elaborated or shown in this Figure.
Fig. 2 diagrammatically shows the elongate anode 3, the array of detectors 9, the object 5 and the object carrier 7, viewed in the longitudinal direction of motion L (see Fig. 1). Furthermore, Fig. 2 shows three diverging X-ray beams I, II and III which are successively generated, each time at a different point of a path f to be followed by the elongate anode 3. These three points 3-1, 3-2, 3-3 are situated at one end, at the centre and at the other end of the path f to be followed by the elongate anode 3. When a plane V is selected in the object 5 at a distance A from the detector array 9, a central point c of the relevant plane is imaged on the detector elements 9-1, 9-2 and 9-3 by the central X-rays from the points 3-1, 3-2 and 3-3, respectively. The distance between the elongate anode 3 and the detector array 9 amounts to D. When the length of the path followed by the anode 3 is f, the distance W between the extreme detector elements 9-1 and 9-3 equals Axf/(D-A).
From the three shadow profiles obtained in the source positions 3-1, 3-2 and 3-3 by detection of the radiation beams I, II and III by the array of detectors 9, a semi-scannogram of the layer V can be constructed in which the parts which are situated in the layer V of the object 5 are clearly shown and the parts of the object which are situated above and below the layer V are blurred. This emphasized imaging of the layer V is achieved by shifting and superposing the three different profiles obtained by means of the measuring beams I, II and III with respect to one another. When the profile I is shifted to the left over a distance equal to half the distance W and the profile III is shifted to the right over a distance equal to half the distance W, the images of the point c of the three profiles will conincide. It can be demonstrated that this also holds good for other points situated in the plane V. It will be apparent that it is also possible to abstain, for example from shifting the profile measured by means of the beam I and to shift the profiles measured by means of the beams II and III over one half W and W, respectively. Generally speaking, when the number of profiles measured in different source positions amounts to N, a profile must be shifted over a distance equal to ixW/(N-1) in order to achieve registration with other profiles, resulting in a semi-scanogram with a better image of the plane V. Therein, i is the profile number measured in the i^th source position, one extreme source position (in this case 3-1 or 3-3) being assigned the index number 0.
Fig. 3 geometrically shows the X-ray source and the array of detectors used to blurr a point in a semi-scannogram which is situated below or above the selected plane. Fig. 3 shows two source positions on the elongate anode 3. The positions, having a spacing f, are the positions 3-1 and 3-3 also used in Fig. 2. Two images of a central point c in the plane V are detected by means of the detectors 9-1 and 9-3, again as shown in Fig. 2. The distance between these two images amounts to W1. For a point P which is situated in a plane W above the plane V there are also formed two images, associated with the source positions 3-1 and 3-2, said images being obtained in the detector positions 9-1P and 9-3P, respectively. The distance between these two images 9-1P and 9-3P amounts to W2. The distance between the anode 3 and the array of detectors 9 amounts to D, the distance between the plane V and the array of detectors is A, and the distance between the plane V to be imaged and the plane W to be blurred is a. The distance W1 between the imaging positions 9-1 and 9-3 amounts to Axf/(D-A). The distance W2 between the two imaging points 9-1P and 9-3P amounts to (A+a)xf/(D(-(A+a)). A blurring factor can now be calculated which indicates the degree of blurring of the plane W. When the blurring factor DF is defined as the difference between W2 and W1, it can be calculated that DF equals fxaxD/(D-A-a)(D-A). It can be deduced therefrom that the blurring DF is more pronounced as the distance f between the extreme source positions 3-1 and 3-3 increases, the distance a between the plane W to the blurred and the desired plane V increases, and the ratio of the distance A between the plane V and the array of detectors 9 and the distance D between the elongate anode 3 and the detector array 9 increases.
The computer tomography device in accordance with the invention offers the advantage that a tomosynthetic scanogram can be made of a plane V where parts of the object situated in this plane are imaged in focus, object parts outside the plane V being imaged in a more or less blurred fashion. The device in accordance with the invention offers other advantages, because during the formation of the tomosynthetic scanogram the anode 3 of the X-ray tube is no longer continuously irradiated in one position, but sequentially in different positions. Because of this movement of the focal spot across the X-ray anode, the energy applied to the anode is distributed among a number of locations, thus reducing the local load of the anode. Local burning of the anode by excessive bombardment with the electron beam is thus avoided. A further advantage is the following. When a scanogram is made according to the state of the art, the failure of one or more detectors will become manifest as straight lines in the scanogram, which lines are reproduced either as completely dark lines or as completely light lines. In the case of failure of a detector in the computer tomography device in accordance with the invention, however, a new calibration can be applied in order to prevent incorrect signals supplied by the faulty detector from spoiling the tomosynthetic scanogram. One of the possibilities of realizing a non-disturbed scanogram in the event of incorrect detector signals is to ignore these signals completely and to standardize the intensity of the signals in the pixels of the scanogram to the number of detectors having contributed to the signal strength in the relevant pixel.
In a computer tomography device comprising an X-ray source having an elongate anode which is irradiated during rotation of the X-ray source around the object in order to realize a tomosynthetic scanogram, the scanning direction of the electron beam across the elongate anode preferably opposes the direction of rotation of the X-ray tube, because the spacing f is then maximum, so that the blurring of the object elements situated outside the plane V is also maximum.

Claims

1. A computer tomography device for determining a radiation attenuation distribution in a traverse slice of an object, which device comprises an X-ray source and detector means for irradiating the object from a plurality of different directions and for detecting the radiation having passed the object, and also comprises an object carrier and displacement means for displacing the object and the object carrier in a direction transversely of the irradiation direction of the X-ray source, characterized in that after a translation of the object, the X-ray source is always situated at the same side of the object so as to irradiate the object from different directions, the device also comprising arithmetic means for combining the detector signals, generated in said different directions, so as to obtain a semi-scannogram in which an object layer is emphasized which is to be selected in advance and which extends substantially transversely of the plane of the irradiation directions.

2. A computer tomography device as claimed in Claim 1, characterized in that the directions in which the object is irradiated are the same after each translation.

3. A computer tomography device as claimed in Claim 1 or 2, characterized in that the translation is a monotonous motion.

4. A computer tomography device as claimed in Claim 1, 2 or 3, characterized in that the X-ray source and the detector means perform a monotonous rotation.

5. A computer tomography device as claimed in Claim 1, 2, 3 or 4, characterized in that the X-ray source is an X-ray tube comprising an elongate anode which extends transversely of the translation direction and which is struck by an electron beam in difference locations.

6. A computer tomography device as claimed in Claim 5, characterized in that the anode is scanned during a rotation of the X-ray source around the object, the scanning direction of the electron beam on the elongate electrode opposing the direction of rotation of the X-ray tube.